Semiconductor device

ABSTRACT

A semiconductor device, such as a memory device or radiation detector, is disclosed, in which data storage cells are formed on a substrate. Each of the data storage cells includes a field effect transistor having a source, drain, and gate, and a body arranged between the source and drain for storing electrical charge generated in the body. The magnitude of the net electrical charge in the body can be adjusted by input signals applied to the transistor, and the adjustment of the net electrical charge by the input signals can be at least partially cancelled by applying electrical voltage signals between the gate and the drain and between the source and the drain.

RELATED APPLICATION

[0001] This patent application is a divisional application of U.S.application Ser. No. 10/450,238 (still pending), filed Jun. 10, 2003.

BACKGROUND

[0002] The present invention relates to semiconductor devices, andrelates particularly, but not exclusively, to DRAM memory devices usingSOI (silicon on insulator) technology.

[0003] DRAM memories are known in which each memory cell consists of asingle transistor and a single capacitor, the binary 1's and 0's of datastored in the DRAM being represented by the capacitor of each cell beingin a charged or discharged state. Charging and discharging of thecapacitors is controlled by switching of the corresponding transistor,which also controls reading of the data stored in the cell. Such anarrangement is disclosed in U.S. Pat. No. 3,387,286 and will be familiarto persons skilled in the art.

[0004] Semiconductor devices incorporating MOSFET (metal oxidesemiconductor field effect transistor) type devices are well known, andarrangements employing SOI (silicon on insulator) are becomingincreasingly available. SOI technology involves the provision of asilicon substrate carrying an insulating silicon dioxide layer coatedwith a layer of silicon in which the individual field effect transistorsare formed by forming source and drain regions of doped silicon of onepolarity separated by a body of doped silicon of the opposite polarity.

[0005] SOI technology suffers the drawback that because the body regionof each individual transistor is electrically insulated from theunderlying silicon substrate, electrical charging of the body can occurunder certain conditions. This can have an effect on the electricalperformance of the transistors and is generally regarded as anundesirable effect. Extensive measures are generally taken to avoid theoccurrence of this effect, as described in more detail in a “Suppressionof parasitic bipolar action in ultra thin film fully depleted CMOS/simoxdevices by Ar-ion implantation into source/drain regions”, published byTerukazu Ohno et al. in IEEE Transactions on Electron Devices, Vol. 45,Number 5, May 1998.

[0006] A known DRAM device is also described in U.S. Pat. No. 4,298,962,in which the DRAM is formed from a plurality of cells, each of whichconsists of an IGFET (insulated gate field effect transistor) formeddirectly on a silicon substrate. This DRAM enables the injection ofcharge carriers from a semiconductor impurity region of oppositepolarity to the polarity of the source and drain regions and which islocated in the source or drain, or the injection of charge carriers fromthe silicon substrate.

[0007] This known device suffers from the drawback that it requires atleast four terminal connections for its operation (connected to thedrain, gate, source and impurity region of opposite polarity or to thesubstrate), which increases the complexity of the device. Furthermore,the memory function of each cell is ensured only while voltages arebeing applied to the transistor source and drain, which affects thereliability of the device, and writing, reading and refreshing of thestored information must be performed in so-called “punch through” mode,which results in heavy power consumption by the device.

[0008] An attempt to manufacture DRAM memories using SOI technology isdisclosed in U.S. Pat. No. 5,448,513. In that known device, each memorycell is formed from two transistors, one of which is used for writingdata to the memory cell, and one of which is used for reading datastored in the device. As a result of each cell consisting of twoseparate transistors, each cell requires four terminal connections forits operation, which increases the complexity of the device, as well asthe surface area necessary for each memory cell as a result of theprovision of two transistors.

[0009] Preferred embodiments of the present invention seek to overcomethe above disadvantages of the prior art.

SUMMARY OF THE INVENTION

[0010] According to an aspect of the present invention, there isprovided a semiconductor device comprising:-

[0011] a substrate;

[0012] at least one data storage cell provided on one side of saidsubstrate, wherein the or each said data storage cell comprises arespective field effect transistor comprising (i) a source; (ii) adrain; (iii) a body arranged between said source and said drain andadapted to at least temporarily retain a net electrical charge generatedin said body such that the magnitude of said net charge can be adjustedby input signals applied to said transistor; and (iv) at least one gateadjacent said body; and charge adjusting means for at least partiallycancelling the adjustment of said net electrical charge by said inputsignals, by applying first predetermined electrical voltage signalsbetween at least one corresponding said gate and the corresponding saiddrain and between the corresponding said source and said drain. Thepresent invention is based upon the surprising discovery that thepreviously undesirable characteristic of excess electrical chargegenerated and retained in the body of the transistor can be used torepresent data. By providing a semiconductor device in which data isstored as an electrical charge in the body of a field effect transistor,this provides the advantage that a much higher level of circuitintegration is possible than in the prior art, since each data cell, forexample when the semiconductor device is a DRAM memory, no longerrequires a capacitor and can consist of a single transistor.Furthermore, by generating said electrical charge in the body of thefield effect transistor (as opposed to in the substrate or in animpurity region provided in the source or drain), this provides thefurther advantage that no specific connection need be made to thesubstrate or impurity region, thus reducing the number of terminalconnections necessary to operate the device.

[0013] In a preferred embodiment, said input signals comprise secondpredetermined electrical voltage signals applied between at least onecorresponding said gate and the corresponding said drain and between thecorresponding said source and said drain. The device may be a memorydevice.

[0014] The device may be a sensor and the charge stored in at least onesaid body in use represents a physical parameter. The input signalscomprise electromagnetic radiation.

[0015] The device may be an electromagnetic radiation sensor.

[0016] The device may further comprise a first insulating layer at leastpartially covering said substrate, wherein the or each said data storagecell is provided on a side of said first insulating layer remote fromsaid substrate.

[0017] The first insulating layer may comprise a layer of semiconductormaterial of opposite doping type to the body of the or each said datastorage cell. By providing a layer of material of opposite doping typeto the transistor body (e.g., a layer of n-type material in the case ofa p-type transistor body), this provides the advantage that by suitablebiasing of the insulating layer such that the body/insulating layerjunction is reverse biased, adjacent transistors can be electricallyisolated from each other without the necessity of usingsilicon-on-insulator (SOI) technology in which a layer of dielectricmaterial such as silicon oxide is formed on a silicon substrate. This inturn provides the advantage that devices according to the invention canbe manufactured using conventional manufacturing techniques.

[0018] The device may further comprise a respective second insulatinglayer provided between at least one said body and/or each correspondingsaid gate.

[0019] In a preferred embodiment, at least one said transistor includesa plurality of defects in the vicinity of the interface between at leastone corresponding said body and the corresponding said second insulatinglayer, for trapping charge carriers of opposite polarity to the chargecarriers stored in the body.

[0020] This provides the advantage of enabling the charge stored in thebody of the transistor to be reduced by means of recombination of thestored charge carriers with charge carriers of opposite polarity trappedin the vicinity of the interface.

[0021] The density of defects in the vicinity of said interface may bebetween 10⁹ and 10¹² per cm².

[0022] The device may further comprise data reading means for causing anelectrical current to flow between a said source and a said drain of atleast one said data storage cell by applying third predeterminedelectrical voltage signals between at least one corresponding said gateand said drain and between said source and said drain.

[0023] The first insulating layer may comprise a plurality of insulatinglayers.

[0024] At least one said data storage cell may be adapted to store atleast two distinguishable levels of said electrical charge.

[0025] In a preferred embodiment, at least one said data storage cell isadapted to store at least three distinguishable levels of saidelectrical charge.

[0026] This provides the advantage that the more distinguishable chargelevels there are which can be used to represent data in a data storagecell, the more bits of data can be stored in each cell. For example, inorder to represent n bits of data, 2^(n) distinguishable charge levelsare required, as a result of which high density data storage devices canbe created.

[0027] At least one said transistor may have a drain/body capacitancegreater than the corresponding source/body capacitance.

[0028] This provides the advantage of reducing the voltages which needto be applied to the transistor to adjust the charge stored in the bodythereof, which in turn improves reliability of operation of the device.

[0029] The body of at least one said transistor may have a higher dopantdensity in the vicinity of said drain than in the vicinity of saidsource.

[0030] The area of the interface between the drain and body of at leastone said transistor may be larger than the area of the interface betweenthe source and the body.

[0031] Common source and/or drain regions may be shared between adjacenttransistors of said device.

[0032] This provides the advantage of improving the extent to which thedevice can be miniaturised.

[0033] According to another aspect of the present invention, there isprovided a method of storing data in a semiconductor device comprising asubstrate, and at least one data storage cell provided on one side ofsaid substrate, wherein the or each said data storage cell comprises arespective field effect transistor comprising (i) a source; (ii) adrain; (iii) a body arranged between said source and said drain andadapted to at least temporarily retain a net electrical charge generatedin said body such that the magnitude of said net charge can be adjustedby input signals applied to said transistor; and (iv) at least one gateadjacent said body; the method comprising the steps of: applying firstpredetermined electrical voltage signals between at least onecorresponding said gate and the corresponding said drain and between thecorresponding said source and said drain to at least partially cancelthe adjustment of said net charge by said input signals.

[0034] The method may further comprise the step of applying secondpredetermined electrical voltage signals between at least one said gateof a said data storage cell and the corresponding said drain and betweenthe corresponding said source and said drain.

[0035] The step of applying second predetermined said electrical signalsmay adjust the charge retained in the corresponding said body by meansof the tunnel effect.

[0036] This provides the advantage of enabling the charge adjustment tobe carried out in a non-conducting state of the transistor in which theonly current is the removal of minority charge carriers from the body ofthe transistor. This in turn enables the charge adjustment operation toinvolve very low power consumption. This also provides the advantagethat a considerably higher charge can be stored in the body of thetransistor since, it is believed, the charge is stored throughoutsubstantially the entire body of the transistor, as opposed to just thatpart of the transistor in the vicinity of the first insulating layer. Asa result, several levels of charge can be stored, representing severalbits of data.

[0037] The charge may be adjusted by the application of a voltage signalbetween at least one said gate and the corresponding drain such that atthe interface between the corresponding body and the drain, the valenceand conduction bands of the body and drain are deformed to injectelectrons from the valence band to the conduction band by the tunneleffect, causing the formation of majority carriers in the body.

[0038] Said charge may be adjusted by means of tunnelling of electronsfrom the valence band to at least one gate of a said field effecttransistor.

[0039] The step of applying first predetermined said voltage signals maycomprise applying electrical voltage signals between at least one saidgate and the corresponding said drain such that at least some of thecharge carriers stored in the corresponding body recombine with chargecarriers of opposite polarity in said body.

[0040] This provides the advantage that the charge stored in theparticular transistor body can be adjusted without the transistor beingswitched into a conductive state, as a result of which the chargeadjustment can be carried out at very low power consumption. Thisfeature is especially advantageous in the case of a semiconductor deviceincorporating a large number of transistors, such as an optical detectorin which individual pixels are provided by transistors.

[0041] The process, operating under the principle known as chargepumping, and described in more detail in the article by G. Groesenekenet al., “A reliable approach to charge pumping measurements in MOStransistors”, IEEE Transactions on Electron Devices, Vol. 31, pp. 42 to53, 1984, provides the advantage that it operates at very low currentlevels, which enables power consumption in devices operating accordingto the process to be minimised.

[0042] The method may further comprise the step of applying at least onesaid voltage signal comprising a first part which causes a conductingchannel to be formed between the source and the drain, the channelcontaining charge carriers of opposite polarity to the charge carriersstored in said body, and a second part which inhibits formation of thechannel, and causes at least some of said stored charge carriers tomigrate towards the position previously occupied by said channel andrecombine with charge carriers of opposite polarity previously in saidchannel.

[0043] The method may further comprise the step of repeating the step ofapplying at least one said voltage signal in a single charge adjustmentoperation sufficiently rapidly to cause at least some of said chargecarriers stored in the body to recombine with charge carriers ofopposite polarity before said charge carriers of opposite polarity cancompletely migrate to said source or said drain.

BRIEF DESCRIPTION OF THE DRAWINGS

[0044] Preferred embodiments of the invention will now be described, byway of example only and not in any limitative sense, with reference tothe accompanying drawings, in which:

[0045]FIG. 1 is a schematic representation of a first embodiments of aMOSFET type SOI transistor for use in a semiconductor device embodyingthe present invention;

[0046]FIG. 2 shows a sequence of electrical pulses to be applied to thetransistor of FIG. 1 to generate a positive charge in the body of thetransistor according to a first method;

[0047]FIG. 3 shows a sequence of electrical pulses to be applied to thetransistor of FIG. 1 to generate a negative charge in the body of thetransistor according to a first method;

[0048]FIG. 4 shows the variation in source-drain current of thetransistor of FIG. 1 as a function of gate voltage, with the body of thetransistor being positively charged, uncharged and negatively charged;

[0049]FIG. 5a is a schematic representation of an SOI MOSFET transistorof a second embodiment for use in a semiconductor device embodying thepresent invention;

[0050]FIG. 5b is a representation of the effect of the application of agate voltage to the transistor of FIG. 5a on the valence and conductionbands of the transistor;

[0051]FIGS. 6a to 6 c illustrate a first method embodying the presentinvention of eliminating a positive charge stored in the body of thetransistor of FIG. 1;

[0052]FIGS. 7a to 7 d illustrate a second method embodying the presentinvention of eliminating a positive charge stored in the body of thetransistor of FIG. 1;

[0053]FIG. 8 is a schematic representation of a SOI MOSFET transistor ofa third embodiment for use in a semiconductor device embodying thepresent invention;

[0054]FIG. 9 is a schematic representation of the gate, source and drainareas of a transistor of a fourth embodiment for use in a semiconductordevice embodying the present invention;

[0055]FIGS. 10 and 11 show multiple charging levels of the transistor ofFIG. 1;

[0056]FIG. 12 shows multiple charging levels of the transistor of FIG. 1achieved by means of the methods of FIGS. 6 and 7;

[0057]FIG. 13 is a schematic representation of part of a DRAM memorydevice embodying the present invention and incorporating the transistorFIGS. 1, 5, 6, 7, 8 or 9;

[0058]FIG. 14 is a schematic representation of part of a DRAM memorydevice of a further embodiment of the present invention andincorporating the transistor FIGS. 1, 5, 6, 7, 8 or 9;

[0059]FIG. 15 is a plan view of the part of the DRAM memory device ofFIG. 14;

[0060]FIG. 16 is a cross-sectional view along the line A-A in FIG. 15;

[0061]FIG. 17 shows the development of integrated circuit processorperformance compared with DRAM performance; and

[0062]FIG. 18 is a schematic representation of an optical sensorembodying the present invention and incorporating the transistor ofFIGS. 1, 5, 6, 7, 8 or 9.

DETAILED DESCRIPTION

[0063] Referring firstly to FIG. 1, an NMOS SOI (silicon on insulator)MOSFET (metal-oxide-silicon field effect transistor) comprises a siliconwafer 10 coated with a layer 12 of silicon dioxide, the wafer 10 andlayer 12 constituting a substrate 13. A layer 14 formed on the substrate13 consists of an island 16 of silicon doped with impurities to form asource 18 on n-type material, a body 20 of p-type material and a drain22 of n-type material, together with a honeycomb insulating structure 24of silicon dioxide, the honeycomb structure being filled by a pluralityof islands 16. The source 18 and drain 22 extend through the entirethickness of the silicon layer 14. An insulating film 26 is formed overbody 20, and a gate 28 of doped semiconductor material is provided ondielectric film 26. The production process steps, chemical compositionsand doping conditions used in manufacturing the transistor of FIG. 1will be familiar to persons skilled in the art, and are also describedin further detail in “SOI: Materials to Systems” by A. J.Auberton-Hervé, IEDM 96. This publication also discloses thattransistors of this type have an electrical instability as a result ofthe fact that the body 20 is electrically floating, and can thereforeacquire an electrical charge, depending upon the sequence of voltagepulses applied to the transistor.

[0064] The transistor shown in FIG. 1 is of the type known to personsskilled in the art as “partially depleted” (PD), in which the depletionregions (i.e., those regions forming junctions between semiconductortypes of opposite polarity and which are depleted of free chargecarriers) do not occupy the entire thickness of the silicon layer 14.

[0065] Referring now to FIG. 2, in order to generate a positive chargein the body of the NMOS transistor of FIG. 1, the gate voltage V_(g) anddrain voltage V_(d), as well as the source voltage, are initially zero.At time t₀, the gate voltage is brought to −1.5V and at time t₀+Δt₀(where Δt₀ can be greater than, less than or equal to zero), the drainvoltage V_(d) is brought to −2V, while the source voltage remains atzero. By applying a negative voltage pulse to the gate and a morenegative voltage pulse to the drain, a concentration of negative chargeforms in the body 20 in the vicinity of the gate 28, while aconcentration of positive charge forms in the body in the vicinity ofinsulating layer 12. At the same time, a conduction channel linking thesource 18 and drain 22 forms in the body 20, allowing conduction ofelectrons between the source 18 and drain 22. This allows electrons tobe attracted into the channel from the source 18 and/or drain 22.

[0066] The application of a negative voltage to the drain 22 relative tothe source as shown in FIG. 2 generates electron-hole pairs by impactionisation in the vicinity of the source. The holes accumulated in thefloating body create a positive charge.

[0067] The drain voltage V_(d) then returns at time t₁ to zero, and thegate voltage V_(g) returns to zero at t₁+Δt₁ to remove the conductivechannel between the source 18 and drain 22, the time interval t₁−t₀typically being between a few nanoseconds and several tens ofnanoseconds, while Δt₁ is of the order of 1 nanosecond. It is alsopossible to create a positive charge in the body 20 by applying apositive drain voltage pulse, depending upon the voltages of the source,drain and gate relative to each other. It has been found in practicethat in order to create a positive charge in the body, the drain voltagemust be switched back to zero before the gate voltage.

[0068] Referring now to FIG. 3, a negative charge is generated in thebody 20 by increasing the gate voltage V_(g) to +1V at while the sourceand drain voltages are held at zero, then reducing the drain voltageV_(d) to −2V at time to +Δt₀ while the source voltage is held at zero.The gate voltage V_(g) and drain voltage V_(d) are then subsequentlybrought to zero at times t₁ and t₁+Δt₁ respectively, where Δt₁ can bepositive or negative (or zero). The application of a positive voltage tothe gate 28 relative to the voltages applied to the source 18 and drain22 again causes the formation of a conductive channel between the source18 and drain 22, as was the case with the formation of an excesspositive charge as described above with reference to FIG. 2. Thepositive voltage applied to the gate 28 also creates a concentration ofnegative charge in the body 20 in the vicinity of the gate 28, and aconcentration of positive charge in that part of the body remote fromthe gate 28, i.e., adjacent the insulating layer 12.

[0069] As a result of the application of the negative voltage to thedrain 22, the body-drain junction is forward biased, as a result ofwhich holes are conducted out of the body 20 to the drain 22. The effectof this is to create an excess of negative charge in the body 20. Itshould be noted that under these bias conditions the generation of holesby impact ionisation is fairly weak. Alternatively, a positive voltagepulse can be applied to the drain and the gate, as a result of which thebody-source junction is forward biased and the holes are removed fromthe body to the source. In a similar way, instead of generating anegative charge in the body 20, a positive charge stored in the body canbe removed.

[0070] Referring now to FIG. 4, the drain current I_(d) is dependentupon the applied gate voltage V_(g), and the Figure shows thisrelationship for a drain voltage V_(d) of 0.3V, the curves 34, 36 and 38representing the body 20 having an excess of positive or negativecharge, or zero excess charge, respectively. It will therefore beappreciated that by the application of calibrated voltages to gate 28and drain 22 and by measuring drain current I_(d), it is possible todetermine whether body 20 is positively or negatively charged, orwhether it is uncharged. This phenomenon enables the transistor of FIG.1 to be used as a data storage cell, different charging levelsrepresenting data “high” and “low” states, or some physical parameter tobe measured, as will be described in greater detail below.

[0071] Referring to FIG. 5a, in which parts common to the embodiment ofFIG. 1 are denoted by like reference numerals but increased by 100, afurther embodiment of an SOI transistor is shown in which the transistoris caused to store a positive charge in its body 120 by means of thetunnel effect. The transistor of FIG. 5a is manufactured by a successionof photo lithographic, doping and etching operations which will befamiliar to persons skilled in the art. The transistor is made to 0.13μm technology with a p-type dopant density of 10¹⁸ atoms per cm³ in thebody 120 and of 10²¹ n-type atoms per cm³ in the drain 122. Theinsulating layer 126 has a thickness of the order of 2 nm.

[0072] In order to operate the transistor of FIG. 5a, the source is heldat 0V, the gate voltage V_(g) is −1.5V and the drain voltage V_(d) is+1V. This causes the tunnel effect at the interface of the body 120 anddrain 122 as a result of the fact that the valence band B_(v) andconduction band B_(c), represented schematically in FIG. 5b, aredistorted. Folding of these bands can be achieved by an electric fieldof the order of 1MV/cm, which results in electrons being extracted bythe drain 122, while the associated holes remain in the body 120. Thisphysical phenomenon is known as “GIDL” (Gate Induced Drain Leakage),described in greater detail for example in the article by Chi Chang etal “Corner Field Induced Drain Leakage in Thin Oxide MOSFETS”, IEDMTechnical Digest, Page 714, 1987.

[0073] The charging operation of FIG. 5a has the advantage over thatdescribed with reference to FIGS. 1 to 3 that the only current flowingduring the charging process is the extraction of electrons from the body120 by the tunnel effect. As a result, charging occurs at very low powerconsumption. Furthermore, it has been found that the charge which can bestored in the body 120 is considerably higher (approximately twice aslarge) than that obtained by previous methods. It is believed that thisis as a result of the fact that a charge is stored throughout the entirevolume of the body 120, not just in that part of the body 120 adjacentto the insulating layer 112.

[0074] It will be appreciated by persons skilled in the art that theprocess of FIG. 5a, which was described with reference to NMOStransistors, can also be applied to PMOS transistors, in which case thegate voltage is positive and the drain voltage negative, and holes areextracted by the drain while electrons are trapped.

[0075] Referring now to FIGS. 6a to 6 c, in which parts common to theembodiment of FIG. 1 are denoted by like reference numerals butincreased by 200, a process is described for removing charge stored inthe body 220 of the transistor. It is important that the body 220 of thetransistor and the insulating film 226 be separated by an interface 230a few atomic layers thick which provides defects forming sites to whichelectrons can attach.

[0076] In order to remove the charge stored in the body 220, a cyclicalsignal shown in the upper part of FIG. 6a is applied to the gate, theinstant illustrated by FIG. 6a being shown by an arrow in the insert.Initially, a potential of 0V is applied to the source 218 and drain 222,and then a potential of 0.8V is applied to gate 228. This has the effectof creating a conducting channel 232 at interface 230, and electrons areattracted into the channel 232 from the source 218 and/or drain 222. Thechannel 232 has a high density of electrons 234, as a result of thepositive voltage applied to gate 228, of which some are attached todefects at the interface 230.

[0077] When a voltage of −2.0V is then applied to gate 228, as indicatedFIG. 6b, the channel 232 disappears, but the bound electrons 234 remainin the interface 230. Moreover, the voltage applied to the gate 228tends to cause holes 236 to migrate towards the interface 230 where theyrecombine with the bound electrons 234. As can be seen in FIG. 6c, whena further cycle is applied beginning with the application of a voltageof 0.8V to gate 228, the channel 232 is again formed. However, comparedto the situation illustrated in FIG. 6a, the number of holes 236 hasdecreased.

[0078] The interface 230 preferably has a defect density between 10⁹ and10¹² per cm², this density and the number of oscillations necessary toremove the particles forming the stored charge representing anacceptable compromise between device performance being limited by thenumber of defects and assisted by the number of trapped electrons. Thepulse duration is typically about 10 ns, the rise and falling time beingof the order of 1 ns. It should also be noted that in certain types oftransistors, it is also possible to form a channel between the source218 and the drain 222 in the vicinity of the insulating layer 212. Insuch a case, the conditions for recombination of charge carriers areslightly different, but the principle of operation is generally thesame.

[0079]FIG. 7a shows a transistor identical in construction to that ofFIGS. 6a to 6 c, but which enables the stored charge to be reduced morerapidly than in the case of FIGS. 6a to 6 c using recombination ofcharges at the interface 230, but without having electrons bound todefects. FIG. 7a shows the state of the transistor before the chargereduction process is commenced, the body 220 having an excess of holes236. By applying a positive voltage, for example 0.8V, to gate 228 asshown in FIG. 7b, while keeping the source and drain at 0V, a channel232 at the interface 230 is created. The channel 232 contains an excessof electrons 234, depending on the positive voltage applied to the gate228, the quantity of free electrons 234 significantly exceeding that ofthe holes 236 present in the body 220 because of attraction of electronsinto the channel 232 from the source 218 and/or drain 222.

[0080] It can be shown that by rapidly reversing the polarity of thesignal applied to the gate 228, for example from 0.8V to −2.0V in a timeof the order of a picosecond, the electrons 234 located in the channel232 do not have time to migrate before the holes 236 contained in thebody 220 arrive in the space previously occupied by the channel 232, asshown in FIG. 7c. The holes 236 and electrons 234 recombine in theinterior of the body 220 without current flowing between the source andthe drain, while the excess electrons 234 migrate towards the source 218and the drain 222. In this way, after a very short period of time, allof the holes 236 of the stored charge are recombined, as shown in FIG.7d.

[0081] In order to achieve the switching speeds necessary for the aboveprocess to be utilized in a semiconductor device, it is necessary toreduce the resistance and parasitic capacitances of the circuits andcontrol lines as far as possible. In the case of memories, this cancause a limitation of the number of transistors per line and per column.However, this limitation is significantly compensated by the significantincreases in the speed with which the stored charge is removed.

[0082] The charge removal process described with reference to FIGS. 6and 7 can be enhanced by providing an asymmetrical source/drain junctionto give larger junction capacitance on the drain side. In thearrangement described with reference to FIGS. 1 to 3, it is observedthat in order to ensure fast writing of data states represented by thecharge level (i.e., in a few nanoseconds), fairly high voltages need tobe used, but that these voltages need to be reduced by deviceoptimization because of reliability problems.

[0083]FIG. 8 shows a further embodiment of a transistor in which thevoltage required to remove charge stored in the body of the transistoris reduced. During discharging of the charged body, pulses are appliedto the drain and to the gate of the transistor so that the body/sourceor body/drain junction is biased in a forward direction. As a result,the majority carriers are removed from the charged floating body,providing a decrease in channel current when the transistor is switchedto its conductive state (see FIG. 4).

[0084] The potential of the floating body can be altered by adjustingthe voltages applied to the transistor contacts, or by altering thebody/source and/or body/drain and/or body/gate capacitances. Forexample, if the potential of the transistor drain is positive comparedto that of the source, the floating body potential can be made morepositive by increasing the capacitance between the drain and thefloating body. In the arrangement shown in FIG. 8, the MOSFET hasdifferent doping profiles for the drain and the source. In particular, aP+ doped region is formed in the vicinity of the drain, which leads toan increased capacitance between the drain and the floating body. Thisis manufactured by adding an implant on the drain side only, and bydiffusing this implant before forming the source and drain implantedregions. An alternative is to increase the capacitive coupling betweenthe drain and the floating body by using different geometries for thedrain and the source, as shown in FIG. 9.

[0085] The improved charging and discharging techniques described withreference to FIGS. 5 to 9 enable significantly greater currentdifferences between the uncharged and highest charged states of thetransistor to be achieved. For example, in the arrangement disclosedwith reference to FIGS. 1 to 3, the current difference between themaximum and minimum charge states is typically 5 to 20 μA/μm of devicewidth. For a 0.13 μm technology, where a typical transistor width of 0.2to 0.3 μm would be used, this means that a current difference of about 1to 6 μA is available. At least 1 μA of current is required to be able tosense the data represented by the charged state.

[0086] The charging and discharging arrangements disclosed withreference to FIGS. 5 to 9 provide a current difference as high as 110μA/μm. The availability 110 μA/μm of signal for devices with 0.2 to 0.3μm width means that current differences of 22 to 33 μA per device can beachieved. As 1 μA is enough for detection, it can be seen that severallevels of charge can be stored in a single transistor body.

[0087] It is therefore possible to store multiple bits of data, forexample, as shown in FIG. 10. FIG. 10a shows a simple arrangement inwhich two levels are available, and one bit of data can be stored. InFIGS. 10b and 10 c, multiple bits of data can be stored in statesbetween the maximum and minimum charging levels. For example, to be ableto store two bits of data, a total current window of 3 μA is required,while 7 μA is required to store three bits per device. With a totalwindow of 33 μA, five bits, corresponding to 32 levels, can be stored inthe same transistor. It will be appreciated that by storing a data wordconsisting of several data bits, as opposed to a single data bit, thestorage capacity of a semiconductor memory using this technique can besignificantly increased.

[0088]FIG. 11 shows the time dependence of a pulsed charging operation.Charging between different levels can be achieved by creating an initial“0” state, and then repeatedly writing “1” pulses, or by starting fromthe highest state, and repeatedly writing “0” pulses. One otherpossibility is to use different writing pulses to obtain differentstates, for example, by varying the writing pulse amplitude and durationto obtain a particular level.

[0089] A further possibility is shown in FIG. 12, which shows the levelsachievable using the charge pumping principle described with referenceto FIGS. 6 and 7. The amount of charge removed after each pulse causes acurrent decrease of ΔI_(S), and the various levels can be obtained bychanging the number of charge pumping pulses.

[0090] As pointed out above, the charge states of the body of thetransistor can be used to create a semiconductor memory device, data“high” states being represented by a positive charge on body 20, anddata “low” states being represented by a negative or zero charge. Thedata stored in the transistor can be read out from the memory device bycomparing the source-drain current of the transistor with that of anuncharged reference transistor.

[0091] A DRAM (dynamic random access memory) device operating accordingto this principle is shown in FIG. 13. A DRAM device is formed from amatrix of data storage cells, each cell consisting of a field effecttransistor of the type shown in FIGS. 1, 5, 6, 7, 8 or 9, the sources ofthe transistors of each row being connected together, and the gates anddrains of the transistors of each column being connected together, atransistor 32 _(ij) corresponding to a transistor located on column Iand row j, the transistor 32 ₂₂ being highlighted in FIG. 13. The gate28, source 18 and drain 22 of transistor 32 _(ij) are connected toconductive tracks 40 i, 42 i and 44 j, respectively. The conductivetracks 40, 42 and 44 are connected to a control unit 46 and a readingunit 48, the construction and operation of which will be familiar topersons skilled in the art. The sources are earthed via the reading unit48, or may be connected to a given fixed potential.

[0092] The operation of the memory device shown in FIG. 13 will now bedescribed.

[0093] Initially, all gates (tracks 40) are at −2V, and all drains(tracks 44) and sources (tracks 42) are held at 0V. In order to write adata bit of state “1” to a transistor 32 _(ij), all tracks 40 of columnsdifferent from i are still held at −2V, while track 40 i is brought to−1.5V. During the time that the potential of track 40 i is −1.5V, alltracks 44 of rows different from j are still held at 0V, while thepotential of track 44 j is brought to −2V. This process generates apositive charge in the body of transistor 32 _(ij), as described abovewith reference to FIG. 2, the positive charge representing a single databit of state “1”. The potential of track 44 j is then brought back to0V, and the potential of track 40 i is subsequently brought back to −2V.

[0094] In order to write a data bit of state “zero” to the transistor 32_(ij), from the condition in which all gates are initially held at −2Vand all sources and drains are held at 0V, track 40 i is brought to avoltage of +1V, the other tracks 40 being held at −2V. During the timethat the potential of track 40 i is +1V, all tracks 44 of rows otherthan j are held at 0V, while the potential of track 44 j is brought to−2V. This generates a net negative charge in the body of the transistorand the potential of track 44 j is then brought back to 0V. Thepotential of track 40 i is then subsequently brought back to −2V.

[0095] In order to read the information out of the transistor 32 _(ij)the voltage of tracks 40 of columns different from i is brought to 0V,while track 40 i is held at 1V, and the voltage of tracks 44 of rowsdifferent from j is brought to 0V, while track 44 j is held at +0.3V. Asshown in FIG. 13, this then enables the current on track 44 j, which isrepresentative of the charge in the body of transistor 32 _(ij), to bedetermined. However, by applying a drain voltage of 0.3V, this alsoprovides the advantage that unlike conventional DRAM devices, thereading of data from transistor 32 _(ij) does not discharge thetransistor 32 _(ij). In other words, because the step of reading datafrom the data storage cell does not destroy the data stored in the cell,the data does not need to be refreshed (i.e., rewritten to thetransistor 32 _(ij)) as frequently as in the prior art.

[0096] However, it will be appreciated by persons skilled in the artthat the electric charge stored in the body of transistor 32 _(ij)decays with time as a result of the electric charges migrating andrecombining with charges of opposite sign, the time dependence of whichdepends on a number of factors, including the temperature of the device,or the presence of radiation or particles such as photons striking thetransistor. A further application of this will be described in moredetail below.

[0097] In the memory unit described with reference to FIG. 13, each datastorage cell is formed by a transistor 32 disposed in an insulatinghoneycomb structure 24. The source and drain of neighbouring transistorsare located adjacent the drain and source of the two neighbouringtransistors in the same row, respectively. A DRAM device of a secondembodiment is shown in FIG. 14, in which parts common to the embodimentof FIG. 13 are denoted by like reference numerals. In the embodiment ofFIG. 14, for each row of transistors, other than those arranged at theends, each transistor shares its drain and source region with itsneighbours. This enables the number of tracks 42 and connections ontracks 44 to be reduced almost by a factor of 2.

[0098] A cross-sectional view of the DRAM device of FIGS. 14 and 15 isshown in FIG. 16, the view being taken along the line A-A in FIG. 15.The device comprises a substrate 13 including a silicon wafer 10 andinsulating layer 12 as in FIG. 1, with sources 18, bodies 20 and drains22 being formed on the insulating layer 12. Dielectric films 26 areprovided on bodies 20, and are extended upwards to the side of gates 28.The gates are interconnected by tracks 40 and the sources 18 areinterconnected via respective pillars 50 by tracks 42, the tracks 40, 42extending parallel to each other in a. direction perpendicular to theplane of the paper of FIG. 16. The drains 22 are interconnected viarespective pillars 52 by tracks 44 extending in a directionperpendicular to tracks 40, 42, and of which only one is shown in FIG.16.

[0099] As will be familiar to persons skilled in the art, in order toperiodically refresh the data contained in the cells of the memorydevice, alternate reading and writing operations can be carried out,with part of the charge detected during reading being supplemented inthe transistor in question. The refreshing frequency typically rangesfrom 1 ms to 1 second, a more detailed description of which is providedin ADRAM circuit design ISBN0-78036014-1.

[0100] As well as using charging of the body of a transistor asdescribed above to construct a DRAM memory device, the charging processcan be applied to other types of memory, such as SRAM (static randomaccess memory). One particular application is to cache SRAMapplications. In modern microprocessors (MPU), the DRAM/MPU performancegap illustrated in FIG. 17 has forced the MPU manufacturers to add somememory to the MPU. This memory is called cache memory. For example, theIntel 486 processor used 8Kbytes of cache memory. This memory is used tostore information that is needed frequently by the MPU. In modernPentium processors, a second level of cache memory, up to 256 Kbytes,has been added to keep up performance. According to industry trends,next generation processors (the 10 Ghz Pentium processors for example)will require a third level of cache memory having a density of 8 to 32Mbytes of cache.

[0101] This memory has previously been provided by a 6 transistor SRAMcell (6T). The cell occupies typically an area of 100 to 150 F², where Fis the minimum feature size, which is quite large. Applying the chargestoring concept set out above, a 1T (1 transistor) cell can replace the6T transistor cell. Integrated in a logic technology, it can occupy a 10to 15 F² area, which is 10 times less. This is of significant importancesince integrating tens of Mbytes of 6T SRAM cells required die sizesmuch too large for practical fabrication.

[0102] As pointed out above, the charge stored on the body of atransistor can also represent some physical parameter to be measured,for example the incidence of optical radiation. FIG. 18 is a schematicrepresentation of a CMOS image sensor embodying the present invention.

[0103] Image sensors have hitherto been made with a matrix ofphotosensitive devices, each of which is provided with a MOS transistoracting as a switch. To boost the information contained in each pixel,the pixel itself is also provided with an in-built amplifier. Suchpixels are called active pixel sensors (APS) and typically includeseveral devices: photo gate APS have typically 1 photosensitivecapacitor and 4 transistors. Photodiode APS have typically 1photosensitive diode and 3 or 4 transistors. In these APS devices theincoming light is incident on the circuit (sometimes through a lens) andhits the sensitive element of the device. An integration cycle thenallows charge generated by the incoming optical radiation to beaccumulated and to generate an electrical signal in a few ms or a fewtens of ms. This signal is then amplified and read. The matrixorganization is similar to a memory matrix organization, a typical pixelsize being about 400 F², where F is the technology minimum feature size.

[0104] In the arrangement shown in FIG. 18, it is possible to create afull pixel with a single transistor that acts at the same time as lightsensitive element and as an amplifier. To achieve this, SOI transistorsare arranged in a matrix arrangement similar to that described for theDRAM applications above. The incoming light can come from the top orfrom the bottom (in this second case, an advantageous feature of SOItechnology being that the silicon substrate below the buried oxide canbe removed locally in the sensor matrix to provide an easy rear sideillumination option).

[0105] To operate the sensor, a reset operation is required, the resetoperation consisting of removing the majority carriers from the floatingbody (holes in the case of an NMOS transistor). For an NMOS device thismeans putting all devices in what is called a “0” state in the DRAMapplication. That this reset operation can be achieved by holeevacuation as described with reference to FIGS. 1 to 3, or morepreferably by the charge pumping technique described with reference toFIGS. 6 and 7. When the reset has been carried out (in typically 1 μs),the light then creates electron hole pairs in the body of the device.The minority carriers are removed through the junction and the majoritycarriers accumulate in the body, allowing the charge integration. Theinformation is read like in a DRAM memory, as explained above. The pixelarea achievable with such devices can be as small as 4F², or 100 timessmaller than in prior art devices. These imagers can be used in variousapplications, such as portable video recorders, digital photography, webcams, PC cameras, mobile telephones, fingerprint identification, and soon.

[0106] It will be appreciated by persons skilled in the art that theabove embodiments have been described by way of example only and not inany limitative sense, and that various alterations and modifications arepossible without departure from the scope of the invention as defined bythe appended claims. For example the process, described with referenceto NMOS transistors, can also be applied to PMOS transistors, in whichcase the stored charge is negative, i.e., formed by electrons, and thatthe free particles in the channel are holes. In that case, the channelis produced by the application of a negative potential to the gate.Also, in certain types of SOI transistors, the substrate can also act asa gate. In that case, the insulating layer performs the function of thedielectric film and the channel is formed at the interface of the bodyand the insulating layer. In addition, the invention can be applied toJFET junction field effect transistor) technology as well as to theMOSFET technology described above. Furthermore, instead of providing alayer of insulating material on the silicon substrate, adjacenttransistors can be electrically isolated from each other by means of alayer of n-type silicon on the silicon substrate, and biasing the n-typesilicon layer such that the junction formed by the p-type transistorbody and the n-type silicon is reverse biased. In such cases, the bodyregion of each transistor should also extend below the correspondingsource and drain regions to separate the source and drain regions fromthe n-type silicon layer, and adjacent transistors are isolated fromeach other by means of a silicon dioxide layer extending downwards asfar as the n-type silicon layer.

1. A semiconductor device comprising a substrate; at least one datastorage cell provided on one side of said substrate, wherein the or eachsaid data storage cell comprises a respective field effect transistorcomprising: (i) a source; (ii) a drain; (iii) a body arranged betweensaid source and said drain and adapted to at least temporarily retain anet electrical charge generated in said body such that the magnitude ofsaid net charge can be adjusted by input signals applied to saidtransistor; and (iv) at least one gate adjacent said body; and chargeadjusting means for at least partially cancelling the adjustment of saidnet electrical charge by said input signals, by applying firstpredetermined electrical voltage signals between at least onecorresponding said gate and the corresponding said drain and between thecorresponding said source and said drain.
 2. A device according to claim1, wherein said input signals comprise second predetermined electricalvoltage signals applied between at least one corresponding said gate andthe corresponding said drain and between the corresponding said sourceand said drain.
 3. A device according to claim 2, wherein the device isa memory device.
 4. A device according to any one of the precedingclaims, wherein the device is a sensor and the charge stored in at leastone said body in use represents a physical parameter.
 5. A deviceaccording to any one of the preceding claims, wherein said input signalscomprise electromagnetic radiation.
 6. A device according to claim 5,wherein the device is an electromagnetic radiation sensor.
 7. A deviceaccording to any one of the preceding claims, further comprising a firstinsulating layer at least partially covering said substrate, wherein theor each said data storage cell is provided on a side of said firstinsulating layer remote from said substrate.
 8. A device according toclaim 7, wherein said first insulating layer comprises a layer ofsemiconductor material of opposite doping type to the body of the oreach said data storage cell.
 9. A device according to any one of thepreceding claims, further comprising a respective second insulatinglayer provided between at least one said body and the or eachcorresponding said gate.
 10. A device according to claim 9, wherein atleast one said transistor includes a plurality of defects in thevicinity of the interface between at least one corresponding said bodyand the corresponding said second insulating layer, for trapping chargecarriers of opposite polarity to the charge carriers stored in the body.11. A device according to claim 10, wherein the density of defects inthe vicinity of said interface is between 10⁹ and 10¹² per cm².
 12. Adevice according to any one of the preceding claims, further comprisingdata reading means for causing an electrical current to flow between asaid source and a said drain of at least one said data storage cell byapplying third predetermined electrical voltage signals between at leastone corresponding said gate and said drain and between said source andsaid drain.
 13. A device according to any one of the preceding claims,wherein said first insulating layer comprises a plurality of insulatinglayers.
 14. A device according to any one of the preceding claims,wherein at least one said data storage cell is adapted to store at leasttwo distinguishable levels of said electrical charge.
 15. A deviceaccording to claim 14, wherein at least one said data storage cell isadapted to store at least three distinguishable levels of saidelectrical charge.
 16. A device according to any one of the precedingclaims, wherein at least one said transistor has a drain/bodycapacitance greater than the corresponding source/body capacitance. 17.A device according to claim 16, wherein the body of at least one saidtransistor has a higher dopant density in the vicinity of said drainthan in the vicinity of said source.
 18. A device according to claim 16or 17, wherein the area of the interface between the drain and body ofat least one said transistor is larger than the area of the interfacebetween the source and the body.
 19. A device according to any one ofthe preceding claims, wherein common source and/or drain regions areshared between adjacent transistors of said device.
 20. A method ofstoring data in a semiconductor device comprising a substrate, and atleast one data storage cell provided on one side of said substrate,wherein the or each said data storage cell comprises a respective fieldeffect transistor comprising (i) a source; (ii) a drain; (iii) a bodyarranged between said source and said drain and adapted to at leasttemporarily retain a net electrical charge generated in said body suchthat the magnitude of said net charge can be adjusted by input signalsapplied to said transistor; and (iv) at least one gate adjacent saidbody; the method comprising the steps of: applying first predeterminedelectrical voltage signals between at least one corresponding said gateand the corresponding said drain and between the corresponding saidsource and said drain to at least partially cancel the adjustment ofsaid net charge by said input signals.
 21. A method according to claim20, further comprising the step of applying second predeterminedelectrical voltage signals between at least one said gate of a said datastorage cell and the corresponding said drain and between thecorresponding said source and said drain.
 22. A method according toclaim 21, wherein the step of applying second predetermined saidelectrical signals adjusts the charge retained in the corresponding saidbody by means of the tunnel effect.
 23. A method according to claim 22,wherein the charge is adjusted by the application of a voltage signalbetween at least one said gate and the corresponding drain such that atthe interface between the corresponding body and the drain, the valenceand conduction bands of the body and drain are deformed to injectelectrons from the valence band to the conduction band by the tunneleffect, causing the formation of majority carriers in the body.
 24. Amethod according to claim 22 or 23, wherein said charge is adjusted bymeans of tunnelling of electrons from the valence band to at least onegate of a said field effect transistor.
 25. A method according to anyone of claims 20 to 24, wherein the step of applying first predeterminedsaid voltage signals comprises applying electrical voltage signalsbetween at least one said gate and the corresponding said drain suchthat at least some of the charge carriers stored in the correspondingbody recombine with charge carriers of opposite polarity in said body.26. A method according to claim 25, further comprising the step ofapplying at least one said voltage signal comprising a first part whichcauses a conducting channel to be formed between the source and thedrain, the channel containing charge carriers of opposite polarity tothe charge carriers stored in said body, and a second part whichinhibits formation of the channel, and causes at least some of saidstored charge carriers to migrate towards the position previouslyoccupied by said channel and recombine with charge carriers of oppositepolarity previously in said channel.
 27. A method according to claim 26,further comprising the step of repeating the step of applying at leastone said voltage signal in a single charge adjustment operationsufficiently rapidly to cause at least some of said charge carriersstored in the body to recombine with charge carriers of oppositepolarity before said charge carriers of opposite polarity can completelymigrate to said source or said drain.